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Proof of The Tracial Algebra of a Noncommutative Law: a Norm-Closed Unital *-Algebra with a Faithful Positive Trace, Determined by Vacuum Vectors, Closed under Square Roots

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After showing that bounded operators agreeing on all polynomial classes coincide and that a vector orthogonal to all classes vanishes (via approximating sequences in the completion), each claim follows from the commutation, adjoint, vacuum and conjugation rules for the GNS multiplication operators, the extension theorem for the complex Hilbert completion, and the square-root theorem.

Proof

Conventions. By The Complex Hilbert Completion is a Complex Hilbert Space Containing a Dense Isometric Image, and Bounded Complex-Linear Maps Extend to It §hilbert, H\mathcal{H} is a complex Hilbert space, so every S∈L(H)S\in\mathcal{L}(\mathcal{H}) has an adjoint S∗∈L(H)S^{*}\in\mathcal{L}(\mathcal{H}) by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint. By the definition of an adjoint in Adjoint of a Linear Map between Complex Inner Product Spaces §adjoint, and because SS is the adjoint of S∗S^{*} by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-calculus,

⟨S∗ξ,η⟩=⟨ξ,Sη⟩and⟨Sξ,η⟩=⟨ξ,S∗η⟩(ξ,η∈H).\langle S^{*}\xi,\eta\rangle=\langle\xi,S\eta\rangle\qquad\text{and}\qquad\langle S\xi,\eta\rangle=\langle\xi,S^{*}\eta\rangle\qquad(\xi,\eta\in\mathcal{H}).

Since ∥S∥op\lVert S\rVert_{\mathrm{op}} is a bound for SS by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §least-bound, linearity gives

(∗)∥Sξ−Sη∥=∥S(ξ−η)∥≤∥S∥op∥ξ−η∥(ξ,η∈H).(\ast)\qquad\lVert S\xi-S\eta\rVert=\lVert S(\xi-\eta)\rVert\le\lVert S\rVert_{\mathrm{op}}\lVert\xi-\eta\rVert\qquad(\xi,\eta\in\mathcal{H}).

All operators LpL_{p}, RpR_{p} below lie in L(H)\mathcal{L}(\mathcal{H}) by Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §multiplication, and sums, scalar multiples and composites of elements of L(H)\mathcal{L}(\mathcal{H}), the zero map and II lie in L(H)\mathcal{L}(\mathcal{H}), a complex vector space in which composition distributes over sums and commutes with scalar multiples, by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §operations.

Preliminary: approximation by classes. Let β=Re⁡hλ\beta=\operatorname{Re}h_{\lambda}. By The Complex GNS Space of a Tracial State on Noncommutative Polynomials §gns and The Hilbert Completion of a Complex Vector Space with a Positive Semidefinite Hermitian Form §completion, H\mathcal{H} is the Hilbert completion HβH_{\beta} of (Pd,β)(\mathcal{P}_{d},\beta) with the same addition and multiplication by real scalars, and its norm is the norm ∣⋅∣|\cdot| of HβH_{\beta} by The Complex Hilbert Completion is a Complex Hilbert Space Containing a Dense Isometric Image, and Bounded Complex-Linear Maps Extend to It §hilbert; so H\mathcal{H} and HβH_{\beta} carry the same metric. Let ξ∈H\xi\in\mathcal{H}. By The Hilbert Completion of a Real Vector Space with a Positive Semidefinite Symmetric Bilinear Form §completion, ξ=[u]\xi=[u] for a β\beta-Cauchy sequence u=(uk)k∈Nu=(u_{k})_{k\in\mathbb{N}} in Pd\mathcal{P}_{d}, and by The Hilbert Completion is a Real Hilbert Space Containing a Dense Isometric Image, and Bounded Linear Maps Extend to It §dense the sequence (Jβuk)(J_{\beta}u_{k}) converges to ξ\xi. Since Jβuk=Jhλuk=uk^J_{\beta}u_{k}=J_{h_{\lambda}}u_{k}=\widehat{u_{k}} by The Hilbert Completion of a Complex Vector Space with a Positive Semidefinite Hermitian Form §canonical-map and The Complex GNS Space of a Tracial State on Noncommutative Polynomials §classes, the classes uk^\widehat{u_{k}} converge to ξ\xi in H\mathcal{H}, that is, ∥uk^−ξ∥→0\lVert\widehat{u_{k}}-\xi\rVert\to0.

(P1) If S,S′∈L(H)S,S'\in\mathcal{L}(\mathcal{H}) and Sq^=S′q^S\widehat{q}=S'\widehat{q} for every q∈Pdq\in\mathcal{P}_{d}, then S=S′S=S'. Let ξ∈H\xi\in\mathcal{H} and let (uk^)(\widehat{u_{k}}) converge to ξ\xi as above. By (∗)(\ast), ∥Suk^−Sξ∥≤∥S∥op∥uk^−ξ∥→0\lVert S\widehat{u_{k}}-S\xi\rVert\le\lVert S\rVert_{\mathrm{op}}\lVert\widehat{u_{k}}-\xi\rVert\to0, so (Suk^)(S\widehat{u_{k}}) converges to SξS\xi; likewise (S′uk^)(S'\widehat{u_{k}}) converges to S′ξS'\xi. These are the same sequence, so Sξ=S′ξS\xi=S'\xi by Uniqueness of Limits in a Metric Space.

(P2) If ζ∈H\zeta\in\mathcal{H} and ⟨ζ,q^⟩=0\langle\zeta,\widehat{q}\rangle=0 for every q∈Pdq\in\mathcal{P}_{d}, then ζ=0\zeta=0. Let (uk^)(\widehat{u_{k}}) converge to ζ\zeta as above. By conditions 2 and 3 of Complex Inner Product Space and by Cauchy-Schwarz Inequality in a Complex Inner Product Space,

∣⟨ζ,uk^⟩−⟨ζ,ζ⟩∣=∣⟨ζ,uk^−ζ⟩∣≤∥ζ∥ ∥uk^−ζ∥→0,\bigl|\langle\zeta,\widehat{u_{k}}\rangle-\langle\zeta,\zeta\rangle\bigr|=\bigl|\langle\zeta,\widehat{u_{k}}-\zeta\rangle\bigr|\le\lVert\zeta\rVert\,\lVert\widehat{u_{k}}-\zeta\rVert\to0,

so the constant sequence ⟨ζ,uk^⟩=0\langle\zeta,\widehat{u_{k}}\rangle=0 converges in C\mathbb{C} (with the metric ∣z−w∣|z-w|) both to 00 and to ⟨ζ,ζ⟩\langle\zeta,\zeta\rangle. By Uniqueness of Limits in a Metric Space, ⟨ζ,ζ⟩=0\langle\zeta,\zeta\rangle=0, and ζ=0\zeta=0 by claim 4 of Elementary Properties of a Complex Inner Product.

1. (Algebra). Recall from The Tracial Algebra of a Noncommutative Law and Its Trace §algebra that M\mathcal{M} consists of the T∈L(H)T\in\mathcal{L}(\mathcal{H}) with TRp=RpTTR_{p}=R_{p}T for all p∈Pdp\in\mathcal{P}_{d}. Clearly IRp=Rp=RpIIR_{p}=R_{p}=R_{p}I, and LpRq=RqLpL_{p}R_{q}=R_{q}L_{p} by Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §commute; so I,Lp∈MI,L_{p}\in\mathcal{M}. Let S,T∈MS,T\in\mathcal{M}, c∈Cc\in\mathbb{C} and p∈Pdp\in\mathcal{P}_{d}. By Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §operations, S+T,cS,ST∈L(H)S+T,cS,ST\in\mathcal{L}(\mathcal{H}) and

(S+T)Rp=SRp+TRp=RpS+RpT=Rp(S+T),(cS)Rp=c(RpS)=Rp(cS),STRp=SRpT=RpST.(S+T)R_{p}=SR_{p}+TR_{p}=R_{p}S+R_{p}T=R_{p}(S+T),\qquad(cS)R_{p}=c(R_{p}S)=R_{p}(cS),\qquad STR_{p}=SR_{p}T=R_{p}ST.

For the adjoint: Rp∗=Rp∗R_{p}^{*}=R_{p^{*}} by Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §adjoint, and RpR_{p} is the adjoint of Rp∗=Rp∗R_{p}^{*}=R_{p^{*}} by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-calculus, so (Rp∗)∗=Rp(R_{p^{*}})^{*}=R_{p} by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-unique. By Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-calculus the composite Rp∗SR_{p^{*}}S has the adjoint S∗RpS^{*}R_{p} and SRp∗SR_{p^{*}} has the adjoint RpS∗R_{p}S^{*}. Since Rp∗S=SRp∗R_{p^{*}}S=SR_{p^{*}}, uniqueness of adjoints (Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-unique) gives S∗Rp=RpS∗S^{*}R_{p}=R_{p}S^{*}; as S∗∈L(H)S^{*}\in\mathcal{L}(\mathcal{H}), S∗∈MS^{*}\in\mathcal{M}.

Now let Tk∈MT_{k}\in\mathcal{M} with Tk→TT_{k}\to T in operator norm, T∈L(H)T\in\mathcal{L}(\mathcal{H}). Using TkRp=RpTkT_{k}R_{p}=R_{p}T_{k} and the operations clause, TRp−RpT=(T−Tk)Rp+Rp(Tk−T)TR_{p}-R_{p}T=(T-T_{k})R_{p}+R_{p}(T_{k}-T), hence by the norm inequalities of Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §operations

∥TRp−RpT∥op≤∥T−Tk∥op∥Rp∥op+∥Rp∥op∥Tk−T∥op=2∥Rp∥op∥Tk−T∥op\lVert TR_{p}-R_{p}T\rVert_{\mathrm{op}}\le\lVert T-T_{k}\rVert_{\mathrm{op}}\lVert R_{p}\rVert_{\mathrm{op}}+\lVert R_{p}\rVert_{\mathrm{op}}\lVert T_{k}-T\rVert_{\mathrm{op}}=2\lVert R_{p}\rVert_{\mathrm{op}}\lVert T_{k}-T\rVert_{\mathrm{op}}

for every kk, using T−Tk=(−1)(Tk−T)T-T_{k}=(-1)(T_{k}-T). The right side tends to 00, so the nonnegative number ∥TRp−RpT∥op\lVert TR_{p}-R_{p}T\rVert_{\mathrm{op}} is at most every positive real and hence is 00 by Comparison of Real Numbers with Arbitrary Positive Slack §vanishing. By Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §least-bound, 00 is then a bound for TRp−RpTTR_{p}-R_{p}T, so ∥(TRp−RpT)v∥=0\lVert(TR_{p}-R_{p}T)v\rVert=0 and (TRp−RpT)v=0(TR_{p}-R_{p}T)v=0 for every v∈Hv\in\mathcal{H} (claim 4 of Elementary Properties of a Complex Inner Product). Thus TRp=RpTTR_{p}=R_{p}T for every pp, and T∈MT\in\mathcal{M}.

2. (Vacuum vectors). Let T∈MT\in\mathcal{M} and q∈Pdq\in\mathcal{P}_{d}. Since RqΩ=q^R_{q}\Omega=\widehat{q} by Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §vacuum, Tq^=TRqΩ=RqTΩT\widehat{q}=TR_{q}\Omega=R_{q}T\Omega.

By Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §conjugation, ⟨Jξ,Jη⟩=⟨η,ξ⟩\langle J\xi,J\eta\rangle=\langle\eta,\xi\rangle and JJη=ηJJ\eta=\eta for all ξ,η∈H\xi,\eta\in\mathcal{H}; applying the first with JηJ\eta in place of η\eta gives

(∗∗)⟨Jξ,η⟩=⟨Jξ,JJη⟩=⟨Jη,ξ⟩(ξ,η∈H).(\ast\ast)\qquad\langle J\xi,\eta\rangle=\langle J\xi,JJ\eta\rangle=\langle J\eta,\xi\rangle\qquad(\xi,\eta\in\mathcal{H}).

Using the conventions, Rq∗=Rq∗R_{q}^{*}=R_{q^{*}} (Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §adjoint), Rq∗Ω=q∗^=Jq^R_{q^{*}}\Omega=\widehat{q^{*}}=J\widehat{q} (Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §vacuum, Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §conjugation) and (∗∗)(\ast\ast),

⟨T∗Ω,q^⟩=⟨Ω,Tq^⟩=⟨Ω,RqTΩ⟩=⟨Rq∗Ω,TΩ⟩=⟨Jq^,TΩ⟩=⟨JTΩ,q^⟩.\langle T^{*}\Omega,\widehat{q}\rangle=\langle\Omega,T\widehat{q}\rangle=\langle\Omega,R_{q}T\Omega\rangle=\langle R_{q^{*}}\Omega,T\Omega\rangle=\langle J\widehat{q},T\Omega\rangle=\langle JT\Omega,\widehat{q}\rangle.

By claims 1 and 2 of Elementary Properties of a Complex Inner Product, ⟨T∗Ω−JTΩ,q^⟩=0\langle T^{*}\Omega-JT\Omega,\widehat{q}\rangle=0 for every qq, so T∗Ω=JTΩT^{*}\Omega=JT\Omega by (P2).

If moreover TΩ=0T\Omega=0, then Tq^=Rq0=0T\widehat{q}=R_{q}0=0 for every qq, so TT and the zero map of L(H)\mathcal{L}(\mathcal{H}) agree on all classes, and T=0T=0 by (P1).

3. (Bounded vectors). Define ϕ:Pd→H\phi:\mathcal{P}_{d}\to\mathcal{H} by ϕ(q)=Rqζ\phi(q)=R_{q}\zeta. By Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §algebra, Rq+q′=Rq+Rq′R_{q+q'}=R_{q}+R_{q'} and Rcq=cRqR_{cq}=cR_{q}, so ϕ\phi is complex-linear. By hypothesis and Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §vacuum,

∥ϕ(q)∥2≤C2∥q^∥2=C2⟨q^,q^⟩=C2λ(q∗q)=C2hλ(q,q).\lVert\phi(q)\rVert^{2}\le C^{2}\lVert\widehat{q}\rVert^{2}=C^{2}\langle\widehat{q},\widehat{q}\rangle=C^{2}\lambda(q^{*}q)=C^{2}h_{\lambda}(q,q).

By The Complex Hilbert Completion is a Complex Hilbert Space Containing a Dense Isometric Image, and Bounded Complex-Linear Maps Extend to It §extension-linear (with V=PdV=\mathcal{P}_{d}, h=hλh=h_{\lambda}, K=HK=\mathcal{H}), there is T∈L(H)T\in\mathcal{L}(\mathcal{H}) with bound CC and Tq^=RqζT\widehat{q}=R_{q}\zeta for every qq; hence ∥T∥op≤C\lVert T\rVert_{\mathrm{op}}\le C by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §least-bound. For p,q∈Pdp,q\in\mathcal{P}_{d}, using Rpq^=qp^R_{p}\widehat{q}=\widehat{qp} (Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §multiplication) and Rqp=RpRqR_{qp}=R_{p}R_{q} (Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §algebra),

TRpq^=Tqp^=Rqpζ=RpRqζ=RpTq^,TR_{p}\widehat{q}=T\widehat{qp}=R_{qp}\zeta=R_{p}R_{q}\zeta=R_{p}T\widehat{q},

so TRp=RpTTR_{p}=R_{p}T by (P1), and T∈MT\in\mathcal{M}. Also TΩ=T1^=R1ζ=ζT\Omega=T\widehat{1}=R_{1}\zeta=\zeta, using The Complex GNS Space of a Tracial State on Noncommutative Polynomials §vacuum and R1=IR_{1}=I (Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §algebra). If T′∈MT'\in\mathcal{M} also satisfies T′Ω=ζT'\Omega=\zeta, then by claim 2, T′q^=RqT′Ω=Rqζ=Tq^T'\widehat{q}=R_{q}T'\Omega=R_{q}\zeta=T\widehat{q} for every qq, so T′=TT'=T by (P1).

4. (Trace). By The Tracial Algebra of a Noncommutative Law and Its Trace §trace, τ(T)=⟨Ω,TΩ⟩\tau(T)=\langle\Omega,T\Omega\rangle, which is linear in TT by conditions 2 and 3 of Complex Inner Product Space (M\mathcal{M} is closed under sums and scalar multiples by claim 1). By Left and Right Multiplication Operators on the Complex GNS Space of a Noncommutative Law: Boundedness, Algebra Rules, Adjoints, Commutation, the Vacuum and the Conjugation §vacuum, τ(I)=⟨Ω,Ω⟩=∥Ω∥2=1\tau(I)=\langle\Omega,\Omega\rangle=\lVert\Omega\rVert^{2}=1 and τ(Lp)=⟨Ω,LpΩ⟩=λ(p)\tau(L_{p})=\langle\Omega,L_{p}\Omega\rangle=\lambda(p).

Let S,T∈MS,T\in\mathcal{M}; then ST,TS,T∗,T∗T∈MST,TS,T^{*},T^{*}T\in\mathcal{M} by claim 1. By the conventions, claim 2 and (∗∗)(\ast\ast),

τ(ST)=⟨Ω,S(TΩ)⟩=⟨S∗Ω,TΩ⟩=⟨JSΩ,TΩ⟩=⟨JTΩ,SΩ⟩=⟨T∗Ω,SΩ⟩=⟨Ω,TSΩ⟩=τ(TS).\tau(ST)=\langle\Omega,S(T\Omega)\rangle=\langle S^{*}\Omega,T\Omega\rangle=\langle JS\Omega,T\Omega\rangle=\langle JT\Omega,S\Omega\rangle=\langle T^{*}\Omega,S\Omega\rangle=\langle\Omega,TS\Omega\rangle=\tau(TS).

By the conventions and condition 1 of Complex Inner Product Space, τ(T∗)=⟨Ω,T∗Ω⟩=⟨TΩ,Ω⟩=⟨Ω,TΩ⟩‾=τ(T)‾\tau(T^{*})=\langle\Omega,T^{*}\Omega\rangle=\langle T\Omega,\Omega\rangle=\overline{\langle\Omega,T\Omega\rangle}=\overline{\tau(T)}. By Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-calculus, τ(T∗T)=⟨Ω,T∗TΩ⟩=∥TΩ∥2≥0\tau(T^{*}T)=\langle\Omega,T^{*}T\Omega\rangle=\lVert T\Omega\rVert^{2}\ge0. If τ(T∗T)=0\tau(T^{*}T)=0, then ⟨TΩ,TΩ⟩=0\langle T\Omega,T\Omega\rangle=0, so TΩ=0T\Omega=0 by claim 4 of Elementary Properties of a Complex Inner Product, and T=0T=0 by claim 2.

5. (Square roots and positivity of the trace). Let T∈MT\in\mathcal{M} with T≥0T\ge0. By Square Roots of Positive Bounded Operators on a Complex Hilbert Space, Commuting with Everything that Commutes with the Operator §square-root there is S∈L(H)S\in\mathcal{L}(\mathcal{H}) with S≥0S\ge0 and SS=TSS=T, and by Square Roots of Positive Bounded Operators on a Complex Hilbert Space, Commuting with Everything that Commutes with the Operator §commutation SS commutes with every element of L(H)\mathcal{L}(\mathcal{H}) that commutes with TT. Each RpR_{p} commutes with TT because T∈MT\in\mathcal{M}, so SRp=RpSSR_{p}=R_{p}S for every pp, and S∈MS\in\mathcal{M}.

Let A,B∈MA,B\in\mathcal{M} with A≥0A\ge0 and B≥0B\ge0, and let S∈MS\in\mathcal{M} with S≥0S\ge0 and SS=ASS=A as just shown. Then SB∈MSB\in\mathcal{M} by claim 1, and by claim 4 applied to SS and SBSB,

τ(AB)=τ(S(SB))=τ((SB)S)=⟨Ω,S(BSΩ)⟩=⟨SΩ,B(SΩ)⟩,\tau(AB)=\tau\bigl(S(SB)\bigr)=\tau\bigl((SB)S\bigr)=\langle\Omega,S(BS\Omega)\rangle=\langle S\Omega,B(S\Omega)\rangle,

the last step because SS is self-adjoint (Self-Adjoint Operator). Since BB is positive semi-definite (Positive Semi-Definite Operator), ⟨SΩ,B(SΩ)⟩\langle S\Omega,B(S\Omega)\rangle is a real number and is ≥0\ge0.

Finally let T∈MT\in\mathcal{M} and A=∥T∥op2I−T∗T∈L(H)A=\lVert T\rVert_{\mathrm{op}}^{2}I-T^{*}T\in\mathcal{L}(\mathcal{H}). By Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-calculus, II is its own adjoint and T∗TT^{*}T is self-adjoint, hence its own adjoint by the same clause and Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-unique; so, again by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-calculus, AA has the adjoint ∥T∥op2I−T∗T=A\lVert T\rVert_{\mathrm{op}}^{2}I-T^{*}T=A (the scalar ∥T∥op2\lVert T\rVert_{\mathrm{op}}^{2} being real), and AA is self-adjoint by the same clause. For v∈Hv\in\mathcal{H}, by conditions 2 and 3 of Complex Inner Product Space and Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-calculus,

⟨v,Av⟩=∥T∥op2∥v∥2−∥Tv∥2,\langle v,Av\rangle=\lVert T\rVert_{\mathrm{op}}^{2}\lVert v\rVert^{2}-\lVert Tv\rVert^{2},

a real number, which is ≥0\ge0 because ∥Tv∥≤∥T∥op∥v∥\lVert Tv\rVert\le\lVert T\rVert_{\mathrm{op}}\lVert v\rVert by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §least-bound. Thus AA is positive semi-definite, and A≥0A\ge0.

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